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Mathematical Methods for Physicists: A concise introduction - Site Map

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COMPLEX INTEGRATION<br />

Solution: For convenience, let z z 0 ˆ re i , where ranges from 0 to 2 as z<br />

ranges around the circle (Fig. 6.7). Then dz ˆ rie i d, and the integral becomes<br />

If n ˆ 0, this reduces to<br />

and if n 6ˆ 0, we have<br />

Z 2<br />

0<br />

rie i d<br />

r n‡1 e ˆ i Z 2<br />

i…n‡1† r n<br />

i<br />

Z 2<br />

0<br />

0<br />

d ˆ 2i<br />

e in d:<br />

Z<br />

i 2<br />

r n …cos n i sin n†d ˆ 0:<br />

0<br />

This is an important and useful result to which we will refer later.<br />

Cauchy's integral theorem<br />

Cauchy's integral theorem has various theoretical and practical consequences. It<br />

states that if f …z† is analytic in a simply-connected region (domain) and on its<br />

boundary C, then<br />

I<br />

f …z†dz ˆ 0:<br />

…6:25†<br />

C<br />

What do we mean by a simply-connected region? A region R (mathematicians<br />

prefer the term `domain') is called simply-connected if any simple closed curve<br />

which lies in R can be shrunk to a point without leaving R. That is, a simplyconnected<br />

region has no hole in it (Fig. 6.7(a)); this is not true <strong>for</strong> a multiplyconnected<br />

region. The multiply-connected regions of Fig. 6.7(b) and (c) have<br />

respectively one and three holes in them.<br />

Figure 6.7.<br />

Simply-connected and doubly-connected regions.<br />

257

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